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               Chapter 3                 EXAMPLE 3.1  S for a phase change
               The Second Law of Thermodynamics
                                            Find  S for the melting of 5.0 g of ice (heat of fusion   79.7 cal/g) at 0°C and
                                            1 atm. Find  S for the reverse process.
                                               The melting is reversible and Eq. (3.25) gives
                                                        ¢H    179.7 cal>g215.0 g2
                                                  ¢S                             1.46 cal>K   6.1 J>K     (3.26)
                                                         T          273 K

                                            For the freezing of 5.0 g of liquid water at 0°C and 1 atm, q  is negative, and
                                                                                               rev
                                             S   6.1 J/K.
                                            Exercise
                                            The heat of vaporization of water at 100°C is 40.66 kJ/mol. Find  S when 5.00 g
                                            of water vapor condenses to liquid at 100°C and 1 atm. (Answer:  30.2 J/K.)



                                                                                                     2
                                         4. Reversible isothermal process. Here T is constant, and  S     T   1  dq
                                                                                                     1       rev
                                                  2
                                             T   1    dq    q /T. Thus
                                                  1  rev   rev
                                                              ¢S   q >T   rev. isotherm. proc.              (3.27)
                                                                    rev
                                             Examples include a reversible phase change (case 3 in this list) and two of the four
                                             steps of a Carnot cycle.
                                         5. Constant-pressure heating with no phase change. First, suppose the heating is
                                             done reversibly. At constant pressure (provided no phase change occurs), dq
                                                                                                             rev
                                                                                     2
                                             dq   C dT [Eq. (2.51)]. The relation  S     dq /T [Eq. (3.21)] becomes
                                               P    P                                1  rev
                                                                  T 2  C P
                                                         ¢S            dT   const. P, no phase change       (3.28)
                                                                T 1  T
                                             If C is essentially constant over the temperature range, then  S   C ln (T /T ).
                                                P                                                      P     2  1

                                         EXAMPLE 3.2  S for heating at constant P

                                            The specific heat capacity c of water is nearly constant at 1.00 cal/(g °C) in the
                                                                   P
                                            temperature range 25°C to 75°C at 1 atm (Fig. 2.15). (a) Find  S when 100 g of
                                            water is reversibly heated from 25°C to 50°C at 1 atm. (b) Without doing the cal-
                                            culation, state whether  S for heating 100 g of water from 50°C to 75°C at 1 atm
                                            will be greater than, equal to, or less than  S for the 25°C to 50°C heating.
                                               (a) The system’s heat capacity is C   mc   (100 g)[1.00 cal/(g °C)]
                                                                              P     P
                                            100 cal/K. (A temperature change of one degree Celsius equals a change of one
                                            kelvin.) For the heating process, (3.28) with C constant gives
                                                                                   P
                                                              T 2 dq rev     T 2 C P   T 2
                                                      ¢S                      dT   C  ln
                                                                                   P
                                                             T 1  T    T 1  T          T 1
                                                                         323 K
                                                            1100 cal>K2 ln       8.06 cal>K   33.7 J>K
                                                                         298 K
                                               (b) Since  C is constant, the reversible heat required for each of the
                                                          P
                                            processes with  T   25°C is the same. For the 50°C to 75°C change, each in-
                                            finitesimal element of heat dq rev  flows in at a higher temperature than for the
                                            25°C to 50°C change. Because of the 1/T factor in  dS   dq /T, each  dq rev
                                                                                                 rev
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